Identities for the trace form of a Lie module #
Let M be a representation of a Lie algebra L over a commutative ring R. Its trace form
B = LieModule.traceForm R L M is symmetric and invariant, B ⁅a, b⁆ c = B a ⁅b, c⁆. Together
with the Leibniz rule those two properties give an identity in four elements,
B ⁅a, b⁆ ⁅c, d⁆ + B ⁅b, c⁆ ⁅a, d⁆ + B ⁅c, a⁆ ⁅b, d⁆ = 0,
which is the Jacobi identity rewritten so that each summand pairs two brackets against each other rather than iterating them. No hypothesis at all is needed on the four elements: this is a consequence of invariance and symmetry, and it holds in every Lie algebra.
Its purpose is downstream: when a, b, c, d are root vectors of a split semisimple Lie
algebra and B is the Killing form, each summand evaluates to a product of two structure
constants weighted by the Killing pairing of an opposite pair of root vectors, and the identity
becomes the four-term relation between the structure constants. Grouping the brackets in pairs is
exactly what makes that evaluation possible, since a summand with an iterated bracket would mix
root spaces of three different roots.
A second, unrelated identity is collected here: over a reduced ring the trace form kills a pair that brackets to zero as soon as one of the two acts nilpotently, because the composite of the two actions is then nilpotent and a nilpotent scalar in a reduced ring is zero. Specialized to the adjoint representation this says that an ad-nilpotent element is Killing-orthogonal to its own centraliser.
Main results #
TauCeti.traceForm_lie_lie_cyclic_eq_zero: the four-element cyclic identity above.TauCeti.traceForm_eq_zero_of_isNilpotent_of_lie_eq_zero: elements bracketing to zero, one of them acting nilpotently, are orthogonal for the trace form.
References #
- R. W. Carter, Simple Groups of Lie Type, §4.1.
- J. E. Humphreys, Introduction to Lie Algebras and Representation Theory, §25.1.
The four-element cyclic identity for an invariant trace form. Pairing the three ways of
splitting a, b, c, d into two brackets, with d always in the second, gives zero.
An element acting nilpotently is orthogonal, for the trace form of any representation, to
everything it brackets to zero with. The trace form pairs x and y by the trace of the
composite of their actions; bracketing to zero in L makes those actions commute, since
toEnd R L M is a morphism of Lie rings, and the trace of a composite with a commuting nilpotent
factor vanishes over a reduced ring.